Photoelectric absorption in semiconductors

Click For Summary

Discussion Overview

The discussion centers on the topic of photoelectric absorption in semiconductors, specifically examining the conservation laws related to momentum and energy during the absorption process. Participants explore the validity of approximations made regarding wave vectors in this context, considering both theoretical and mathematical perspectives.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant questions the validity of neglecting the wave vector of the incoming photon (kph) in the conservation law, suggesting that this assumption may only hold when electrons are at the edge of the Brillouin Zone, while near the Γ-point, kph could be comparable to the electron wave vectors (ki and kf).
  • Another participant suggests performing calculations and sketching the photon and electron dispersion to illustrate the validity of the professor's approximation across different scenarios.
  • A third participant highlights the need to consider both momentum and energy conservation in the context of the discussion.
  • One participant clarifies that the conservation law applies only to in-plane momentum, indicating that out-of-plane momentum introduces additional complexity.
  • A participant presents calculations based on energy conservation, relating the energy of the photon to the band gap (Egap) and deriving a relationship for kph, questioning whether their reasoning justifies the assumption that kph can be approximated as zero.
  • Another participant reflects on their calculations, suggesting that they may have overcomplicated the math while reiterating the relationship between the wave vectors and the dimensions of the Brillouin zone.

Areas of Agreement / Disagreement

Participants express differing views on the validity of approximations regarding kph and its implications for momentum conservation. There is no consensus on the conditions under which these approximations hold true, indicating ongoing debate and exploration of the topic.

Contextual Notes

Participants note that the assumptions made regarding the neglect of kph depend on the specific conditions of the electron states involved, particularly their proximity to the Brillouin Zone edges or the Γ-point. The discussion also highlights the complexity introduced by out-of-plane momentum considerations.

MicheleC88
Messages
4
Reaction score
0
Hi everybody. I'm new here and, first of all, sorry for my bad english :-D

I'm studying photoelectric absorption in semiconductors.
The book (and professor too) says that, in the conservation law:

ki + kph = kf

(where ki and kf are wave vectors of initial and final electron state, and kph is the wave vector of incoming photon) we can neglect kph because it is ≈ 2π/λ, whereas ki and kf are ≈ 2π/a, and λ>>a. (a is the length of unitary cell in real space).
But I think that this assumption is good only if electron is at the edge of Brillouin Zone; if the initial and final electrons are near \Gamma-point, they should have a very little wave vector, comparable with kph, making the approximation not valid.

what is wrong in my words?
 
Physics news on Phys.org
Just do the math once and sketch the photon dispersion (energy versus k) and the electron dispersion (crystal electron or for simplicity even a free one) into the same graph with the correct dimensions. This is pretty instructive and will give you a good argument for why the approximation your professor gave you is a very good one pretty much everywhere.
 
So, I think having understood from your words, the key is that the conservation of momentum has to be combined with the conservation of energy?
 
Actually, that conservation law is valid only for the in-plane momentum, i.e. parallel to the surface of the material. The out-of-plane momentum is way more complicated than that.

Zz.
 
I tried to make the following math.
from energy conservation: Eph≈Egap
(assuming that initial and final electrons are in proximity of, respectively, the maximum of VB and minimum of CB)

We know that kph = ω/c = Eph/(\hbarc)

So, from momentum conservation law:

|kf - ki | = |kph|≈Egap/(\hbarc)

Doing the calc (i assumed 1 eV for Egap):
|kf - ki | ≈ 10-4 angstrom-1, which is about 1 part of thousand of tipical size of Brillouin zone.

Are my reasoning correct to justify the assumpion kph=0 ?
 
Last edited:
However, I think I made the math more complex than necessary:

ki - kf = kph = \frac{2π}{λ}\widehat{k}_{ph}

(ki - kf) / (size of Brillouin zone) = \frac{2π}{λ}\frac{a}{2π}\widehat{k}_{ph} << 1 \cdot \widehat{k}_{ph}

Thanks to all for the reply!
 

Similar threads

Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
4K